Optical electric field sensor

Abstract: The present invention provides amino alcohols dehydrogenases which catalyze a reaction to produce keto alcohols, ketones, aldehydes, keto acids from corresponding amino alcohols, amines, and amino acids in the presence of NAD + , and a reaction to produce amino alcohols, amines, amino acids from corresponding keto alcohols, ketones, aldehydes, and keto acids in the presence of NADH and ammonium ions. Also provided is a method for producing the enzymes and uses of the enzyme. The enzymes of the present invention can be obtained from microorganisms belonging to the genera Streptomyces, Pseudomonas, Burkholdenia , or Arthrobacter.

Description: (Technical Field) This invention relates to an optical electric field sensor for use in measurement of an electric field intensity within a spatial field, typically, in EMC measurement (noise measurement). (Background Art) An optical waveguide Mach-Zehnder interferometer has a structure in which an optical waveguide is branched and one or both of the branched optical waveguides are applied with an electric field parallel to a crystal axis thereof to phase-shift light beams propagating therein, which beams are thereafter combined again. Because after the combination, a light intensity is varied by the electric field applied thereto, the interferometer is used as an electric field sensor for detecting, by measurement of the light intensity, an electric field intensity applied to antennas connected to electrodes. The document US-A-5 210 407 shows such an electric field sensor. The intensity of an outgoing light beam of the Mach-Zehnder interferometer exhibits a trigonometric function wave curve with respect to the electric field applied to the electrodes. Fig. 1(a) shows one example of a conventional optical electric field sensor. As illustrated in the figure, the optical electric field sensor comprises an optical branched waveguide type interferometer formed on a LiNbO 3 substrate by diffusion of Ti. One of the two branched optical waveguides is provided with electrodes to form an optical modulator. The optical modulator is fixedly housed in a case 1 made of plastic. The electrodes of the optical modulator are connected to antennas 2, respectively. A polarization maintaining fiber 3 and a single mode fiber 4 are connected to a light incident side and a light outgoing side of the optical modulator,' respectively. An electric field spontaneously or forcedly generated is transmitted through the antennas to the electrodes to produce phase modulation in the optical waveguide. The light beam combined thereafter is modulated in intensity and, thus, has the light intensity corresponding to the electric field. Fig. 2 shows a conventional optical waveguide Mach-Zehnder interferometer used in the optical modulator illustrated in Fig. 1(a). As illustrated in Fig. 2, the optical waveguide Mach-Zehnder interferometer has a structure such that an optical waveguide is branched into branched optical waveguides 12 and 12, one or both of which are applied with an electric field parallel to an optical axis through modulation electrodes 22 and 22 to provide phase-shift in the optical waveguides before combined again. Because a light intensity after combined is varied by the electric voltage applied thereto, the interferometer can be used as an electric field sensor for detecting, by measurement of the light intensity, an electric field intensity applied to antennas 2 as a low voltage applied across the modulation electrodes 22 and 22. Fig. 3 shows an optical modulation characteristic of the Mach-Zehnder interferometer illustrated in Fig. 2. As illustrated in Fig. 3, an output intensity (relative intensity) of the light beam modulated in intensity by the Mach-Zehnder interferometer varies along a trigonometric function wave (sine wave) curve with respect to the applied voltage. In view of the above, adjustment (optical bias adjustment) is performed so that the light intensity is located at a linear variation point (a middle point between the maximum level and the minimum level) of the trigonometric function wave when the applied voltage is equal to 0V. In this event, variation in light intensity and the applied electric field exhibit a proportional relationship. It is therefore possible, as an electric field sensor, to measure the applied electric field by the light intensity. In other words, such a characteristic is required for use as an electric field sensor. The conventional optical electric field sensor, however, has a distance between the electrodes which is as small as several microns. If foreign substances, such as alkali ions, exist between the electrodes, the voltage applied across the electrodes is accumulated as a charged voltage. This results in fluctuation of an optical modulation ratio with respect to the applied voltage. Such fluctuation tends to occur in a low frequency rather than in a high frequency (DC drift, giving a largest influence upon a direct-current voltage). In that event, measurement accuracy of the optical electric field sensor is deteriorated. When the optical electric field sensor of this type is subjected to temperature variation, carrier particles are generated within a crystal, moved, and nonuniformly accumulated in the vicinity of the electrodes to produce an internal electric field. This results in instability (temperature drift) of the outgoing light beam. Such fluctuation in characteristic is great and small when the temperature variation is drastic and gentle, respectively. The temperature drift will briefly be described in conjunction with Fig. 1(b) and Fig. 1(c). Referring to Fig. 1(b), the optical electric field sensor is put in a condition where an ambient temperature is equal to 30°C which is higher than a room temperature. An incident light beam is incident to the polarization maintaining fiber 3 (Fig. 1(a)) and passes through the conventional optical electric field sensor to be emitted from the single mode fiber 4 as a normal output light beam having a waveform A. An abscissa and an ordinate represent an applied electric field and a light intensity, respectively. Herein, adjustment is made so that the light intensity is located at a middle point between the maximum level and the minimum level when the electric field applied to the antennas is equal to 0 (V). As far as a normal operation is carried out, the waveform is as illustrated in Fig. 1(b). When subjected to the temperature drift, the output light beam emitted from the single mode fiber 4 has a waveform B illustrated in Fig. 1(c). In the waveform B, the light intensity is phase-shifted by π/4 with respect to the waveform A of the incident light beam when the electric field applied to the antennas is equal to 0 (V). Such shift is the temperature drift which deteriorates the temperature characteristic of the optical electric field sensor. As a result, the sensitivity becomes unstable. In order to improve the temperature characteristic, the optical modulator used in the conventional optical electric field sensor adopts a method of indirect compensation. Specifically, the optical crystal is given distortion equal in magnitude and reverse in polarity to the drift by, for example, application of a physical stress caused by a Peltier element or the like, and alternatively, addition of an extra electric field reverse to the distortion the modulation electric field. However, there has been no such optical electric field sensor that has a structure for suppressing heat conduction to the optical modulator, which heat conduction substantially is a cause of deterioration of the temperature characteristic. In order to monitor the output of the optical modulator, to measure the temperature drift, and to apply distortion for compensating it as described above, a device for operating these mechanisms is required. Furthermore, an accuracy is required. On the other hand, when the above-mentioned Mach-Zehnder interferometer is manufactured, the optical modulation characteristic with respect to the applied voltage generally changes in dependence upon the characteristic of the LiNbO 3 substrate or the manufacturing condition of the element. Specifically, it is possible to assure a reproducibility of those characteristics such as a half-wavelength voltage and a loss. However, it is difficult to adjust the light intensity at the applied voltage of 0V to the middle point between the maximum level and the minimum level as required to the electric field sensor. In view of the above, it is a general practice to carry out adjustment (optical bias adjustment) by giving distortion to the waveguide after manufactured. In the meanwhile, the electric field sensor has a structure in which the antennas made of metal receive the electric field to generate the applied voltage at the electrode portions of the optical modulator. When any metal other than the antenna is present around the sensor, the electric field generated around the electric field sensor is disturbed. Therefore, the package is preferably made of a nonmetallic material to remove metal components other than the antennas. Use is generally made of resin such as plastic. The electric field sensor thus manufactured is used to measure the electric field intensity on the order of several mV/m because of its characteristic, and is readily subjected to the influence of the electric field generated therearound. In addition, the package made of resin such as plastic generates an electrostatic field having such a level that fluctuates the optical bias. Since the electrostatic field generated by the package is greatly concerned with variation of humidity or the like, it is difficult to provide an element having a constant optical bias. However, in order to compensate for deviation of the optical bias due to the electrostatic field, consideration has mainly been directed to adjustment of the optical bias after packaging. An optical electric field sensor according to the preamble of claim 1 can be derived from US patent 5,210,407. It is an object of this invention to provide an optical electric field sensor which is capable of inhibiting interference with an external environment to readily prevent invasion of dirt or foreign substances by applying an agent having a stable characteristic on an area between electrodes where invasion of the foreign substances is otherwise easy. It is a further object of this invention to provide an optical electric field sensor having a structure of removing an electrostatic field generated by a package material after packaging to thereby avoid disturbance of an electric field to be measured. According to this invention, there is provided an optical electric field sensor which comprises at least a pair of modulation electrodes located in the vicinity of an optical waveguide formed on an optical crystal substrate having an electrooptical effect and which is for measuring an electric field intensity by the use of variation of at least one of an intensity, a phase, and a polarization direction of a light beam that is caused by leading to the pair of modulation electrodes an electric field spontaneously or forcedly generated, wherein conductive resin is applied onto the entire surface of the optical crystal substrate and/or silicone is applied between the modulation electrodes. Specifically, according to this invention, a conductive resin film is used as the conductive film and a structure is used where the conductive film is applied onto the entire surface of the crystal substrate to cause migration and cancellation of unstable electric charge produced by temperature variation.. The conductive film used must be carefully selected in respect of a resistance and a material so as not to affect the drift. According to this invention, silicone is used. This agent is excellent in isolation from the external environment, rapid in drying, and easy in application. In addition, the agent itself does not act as a foreign substance causing voltage fluctuation because of absence of any undesired unstable ions. Thus, it is noted that the agent is reliable for a long time. According to this invention, it is preferable that the optical crystal substrate is fixedly surrounded by a heat insulation material. Specifically, according to this invention, the optical modulator is fixedly housed in a case made of a heat insulation material such as a low heat conduction material, a foam-containing material, and a low heat conduction and foam-containing material. Alternatively, a case in which the optical modulator is fixedly housed is covered with a heat insulation material. Thus, heat conduction from the outside of the optical modulator is suppressed. (Brief Description of the Drawing) Fig. 1(a) is a view illustrating a structure of a conventional optical electric field sensor; Figs. 1(b) and (c) are views for describing an influence of a temperature upon a relationship between a light intensity and an electric field in the optical electric field sensor in Fig. 1(a); Fig. 2(a) is a plan view of the optical electric field sensor illustrated in Fig. 1(a): Fig. 2(b) shows a relationship between the time and the light intensity of an input light beam in the optical electric field sensor in Fig. 2(a); Fig. 2(c) shows a relationship between a voltage of an electric field signal and the time in the optical electric field sensor in Fig. 2(a); Fig. 2(d) shows a relationship between the time and the light intensity of an output light beam in the optical electric field sensor in Fig. 2(a); Fig. 3 shows an optical modulation characteristic with respect to an applied voltage in the optical electric field sensor in Fig. 2; Fig. 4 is a perspective view illustrating a structure of an optical electric field sensor according to a second example not representing this invention but useful for its understanding with an upper half of a package removed; Fig. 5(a) shows an optical electric field sensor according to a third example not representing this invention, but useful for its understanding; Figs. 5(b) and (c) are views for describing an influence of a temperature upon a relationship between a light intensity and an electric field in the optical electric field sensor in Fig. 5(a); Fig. 6(a) is a plan view of an optical electric field sensor according to a first embodiment of this invention; Fig. 6(b) is a sectional view of the optical electric field sensor in Fig. 6(a) taken along a line A-A'; Fig. 7 shows a relationship between an applied voltage and an output light beam in the optical electric field sensor in Fig. 6; Fig. 8(a) is a plan view of an optical electric field sensor according to a second embodiment of this invention; Fig. 8(b) is a sectional view of the optical electric field sensor in Fig. 8(a) taken along a line B-B'; Fig. 9 shows a relationship between an applied voltage and an output light beam in the optical electric field sensor illustrated in Figs. 8(a) and (b); and Fig. 10 shows an optical electric field sensor according to a fourth example not representing this invention, but useful for its understanding (Best Mode for Embodying the Invention) Now, description will be made in detail with reference to the accompanying drawings. An optical electric field sensor according to a first example not representing this invention but useful for its understanding has a structure similar to that of the conventional optical electric field sensor illustrated in Fig. 1(a) except that a case 1 is made of glass instead of plastic in the conventional example. Specifically, the optical electric field sensor comprises an optical branched waveguide type interferometer formed on an LiNbO 3 substrate by diffusion of Ti. One of two branched optical waveguides is provided with electrodes. This optical modulator is fixedly housed in the glass case. The electrodes of the optical modulator are connected to antennas 2, respectively. A polarization maintaining fiber and a single mode fiber are connected to a light incident side and a light outgoing side of the optical modulator, respectively. When the optical electric field sensor having the above-mentioned structure according to the first embodiment is put in an environment of 30°C which is higher than the room temperature, no fluctuation in optical modulation characteristic is observed. Fig. 4 is a slightly perspective view of an optical electric field sensor according to the second example with an upper half of a quartz package removed. A Mach-Zehnder interferometer pattern was formed on a Z-cut substrate 11 (having a crystal axis in a Z direction) of LiNbO 3 by a Ti pattern. Then, optical waveguides 12 were formed by thermal diffusion. Thereafter, an SiO 2 film was formed on a surface on the optical waveguides 12. Modulation electrode patterns 13 were formed thereon. For input and output of a laser beam, the optical waveguide 12 was subjected to face polishing. A constant polarization optical fiber 3 and a single mode fiber 4 were connected to a light incident side and a light outgoing side, respectively. Those elements thus manufactured had the optical modulation characteristics as illustrated in Fig. 2 and described in the foregoing. Selection was made of an optimum one as an optical electric field sensor. Thereafter, antennas 2 for electric field detection were connected to modulation electrodes 13. An entire arrangement was housed in the quartz package 7. The package was made up by the use of an organic adhesive and sealed so that the internal element is not affected by an outside air. For the sake of comparison, a conventional optical electric field sensor was prepared by the use of a package made of acrylic plastic. It was noted here that those elements were selected to have a same optical modulation characteristic. In order to demonstrate the effect of this example, each element was wrapped by acrylic sponge and left at the room temperature for one day with the electrodes short-circuited, so as to generate an electrostatic field by the package. Then, the optical modulation characteristic of each optical electric field sensor was measured. In the conventional optical electric field sensor, fluctuation of the optical bias was observed. On the other hand, no fluctuation was found in the optical electric field sensor of this invention. With respect to variation of the ambient temperature, no fluctuation of the optical bias was observed in the optical electric field sensor of this invention using the quartz package even in a condition (10°C higher than the room temperature) where fluctuation of the optical bias is caused in the conventional optical electric field sensor with the package made of acrylic plastic. Similar comparison was made as regards another optical electric field sensor according to this invention. In this optical electric field sensor, the quartz package was subjected to the abrasion process. In this event, a more excellent result was obtained as compared with the above-mentioned case. With the package made of ceramics, a similar result was obtained as in case of quartz. By the use of the package made of glass (quartz) or ceramics, the above-mentioned optical electric field sensor according to the second embodiment of this invention achieves stable characteristics without variation of the optical modulation characteristic after assembling and without fluctuation of the optical bias in response to the temperature variation from the room temperature. Because heat insulation of the element is stable in the optical electric field sensor according to the first embodiment of this invention, no consideration is required of the influence of the temperature drift as far as it is used at the room temperature (mainly used in an EMC measurement within a radio dark room, which is carried out in an environment of the room temperature). It is therefore possible to provide an optical electric field sensor manufactured with a high productivity by removing a process for making any way against the temperature drift. By the use of such a technique in the second example, no electrostatic field is generated by the package material and the influence of the variation of the ambient temperature upon variation of the temperature within the package is reduced. Fig. 5 shows an electric field sensor according to the third example. As illustrated in Fig. 5, an optical branched waveguide type interferometer is prepared on an LiNbO 3 substrate by diffusion of Ti. One of two branched optical waveguides is provided with electrodes. This optical modulator is fixedly housed in a glass case 1. The electrodes of the optical modulator are connected to antennas 2. A polarization maintaining fiber 3 and a single mode fiber 4 are connected to a light incident side and a light outgoing side of the optical modulator, respectively. A combination of those components forms the optical electric field sensor. In Fig. 5, the optical electric field sensor is put in a condition where the ambient temperature of the optical electric field sensor is 30°C. A light beam is incident to the polarization maintaining fiber 3 and passes through the optical electric field sensor to be emitted from the single mode fiber 4 as a normal outgoing light beam having a waveform C. An abscissa and an ordinate represent an applied electric field and a light intensity, respectively. Herein, adjustment is made so that the light intensity is located at a middle point between the maximum level and the minimum level when the electric field applied to the antenna is equal to 0 (V). The foregoing structure is similar to that of the first example. The optical electric field sensor according to the third example is different from the first example in that it is covered by expanded polystylene foam 5 having a heat insulation effect. In the optical electric field sensor according to the third example, a light beam is incident to the polarization maintaining fiber 3 and passes through the optical electric field sensor to be emitted from the single mode fiber 4 as a normal outgoing light beam having a waveform C as illustrated in Fig. 5(b). Adjustment of a zero point is carried out so that the light intensity is located at a middle point between the maximum level and the minimum level when the electric field applied to the antenna is equal to 0 (V), as is similar to the conventional case. However, as illustrated in Fig. 5(c), a difference exists in that a waveform D of the outgoing light beam emitted from the single mode fiber 4 is coincident with the waveform C without being subjected to the temperature drift. Specifically, in the waveform D, the light intensity is equal to 0 (V) when the electric field applied to the antennas is equal to 0 (V). Thus, the waveform is not varied from the waveform C of the normal outgoing light beam. As described, the expanded polystylene foam 5 suppresses the temperature drift (see Fig. 1(c)) of the optical electric field sensor to achieve an excellent temperature characteristic and a stable sensitivity. From the above-mentioned result, it is understood that the optical electric field sensor using a material having a heat insulation effect according to the third example can suppress the influence of the temperature drift resulting from variation of the ambient temperature to improve a temperature characteristic and to keep a stable sensitivity of the sensor. According to the third example, the influence of variation of the ambient temperature of the optical electric field sensor upon the optical crystal of the optical modulator is suppressed to be small. It is therefore possible to provide an optical electric field sensor having an excellent temperature characteristic. According to the third example, it is possible not only to contribute to the improvement of the temperature characteristic of the optical electric field sensor, which is a problem in prior art, but also to provide an optical electric field sensor manufactured at a relatively low cost in a reduced process time with a high productivity. (First Embodiment) Fig. 6 shows a main portion of an optical electric field sensor according to a first embodiment of this invention. As illustrated in Fig. 6, a Ti (film thickness of 80 nm (800 Å)) thermal diffusion optical waveguide (hereinafter simply called an optical waveguide) 12 was formed on a X-cut substrate 11 of LiNbO 3 crystal as a branch interference type optical waveguide which is branched and again joined together. Modulation electrodes 13 were arranged in an area after branched and before joined again. Thus, a Mach-Zehnder optical interferometer 20 was manufactured. On opposite ends of the element, two short dipole antennas (not shown) of 75mm were connected to the modulation electrodes 13 in the manner similar to Fig. 2. A constant polarization optical fiber and a single mode optical fiber were connected to a light input side and a light output side, respectively (not shown). An input light beam was a laser light beam having a wavelength of 1.3 µm. An output light beam was subjected to O/E conversion for measurement. A direct current voltage was applied to the short dipoles of the optical electric field sensor thus manufactured. A half-wavelength voltage V π was obtained from the intensity variation of the optical output in response to the applied voltage. By the use of a conductive spray of this invention, a conductive resin film 14 was formed (process time being on the order of 5 seconds per one) on the optical modulator portion of the optical electric field sensor thus manufactured. In a thermostatic chamber, variation of the intensity of the outgoing light beam in response to temperature variation was confirmed. The temperature was varied stepwise by 10°C in a range between -10°C and 60°C. For the sake of comparison, a similar test was carried out for the optical electric field sensor without treatment by the conductive spray. The test data were dealt with in the form of voltage shift which is obtained from the light intensity with reference to an SG curve 25 in Fig. 7 and normalized by the half-wavelength voltage V. The optical electric field sensor without using the conductive spray was unstable in light intensity, the level of which fluctuated even around 25°C. With respect to the temperature variation, a shift not smaller than the half-wavelength voltage was confirmed. On the other hand, the optical electric field sensor according to this invention exhibited no variation in light intensity even around 25°C. It was confirmed that the shift in the optical bias is not greater than ±0.3% (normalized by the half-wavelength voltage) in an environment of the temperature between -10°C and 60°C. The above-mentioned result shows that the first embodiment of this invention is effective in improvement of the temperature characteristic of the optical electric field sensor. Also from the first embodiment, it is confirmed that this invention greatly contributes to improvement of productivity because manufacture is easily carried out at a very low cost as compared with the conventional case. Accordingly, it is found out that the first embodiment of this invention provides an optical electric field sensor with a conductive film formed by an inexpensive and simple process. (Second Embodiment) Fig. 8 shows a main portion of an optical electric field sensor according to a second embodiment of this invention. As illustrated in Fig. 8, a Ti (film thickness of 80 nm (800 Å)) thermal diffusion optical waveguide 12 was formed on a X-cut substrate 11 of LiNbO 3 crystal as a branch interference type optical waveguide which is branched and again joined together. Modulation electrodes 13 were formed in an area after branched and before joined again. Thus, a Mach-Zehnder optical interferometer was manufactured in the manner similar to the fourth embodiment. In the second embodiment, silicone 17 was applied onto a region including the modulation electrodes 13 adjacent to the optical waveguide 12. On opposite ends of the element, two short dipole antennas of 75mm were connected to the modulation electrodes 13. A constant polarization optical fiber and a single mode optical fiber (not shown) were connected to a light input side and an output side, respectively. An input light beam was a laser light beam having a wavelength of 1.3 µm. An output light beam was subjected to O/E conversion for measurement. A direct current voltage was applied to the short dipoles of the optical electric field sensor thus manufactured. A half-wavelength voltage V π was obtained from the intensity variation of the optical output in response to the applied voltage. The result was illustrated in Fig. 9. The optical electric field sensor thus manufactured was applied with a DC voltage (12V), which tends to cause characteristic deterioration, and left for 100 hours. Then, the DC drift was measured. Likewise, the sample without being applied with silicone was measured for comparison. After measurement, a test was carried out for 100 hours at a constant temperature and humidity of 60°C and 60% which was a bad environment realized by the use of common tap water for humidification. Then, the DC drift was similarly measured. As a result, the time period until the initial DC drift is caused was unchanged in the sample applied with the silicone. On the other hand, the time period was reduced more than 10 times in the sample without being applied with the silicone. According to the fifth embodiment of this invention, the agent having a stable characteristic, namely, having no undesired ions and a high reliability, is applied in an area between the electrodes, where any foreign substance tends to invade. It is therefore possible to provide an optical electric field sensor which is capable of inhibiting interference with an external environment to readily prevent invasion of dirt or a foreign substance. It is confirmed that, by the use of the optical electric field sensor according to the second embodiment of this invention, a stable optical electric field sensor is provided which can suppress variation of the DC drift although a process is very simple. In addition, according to the second embodiment of this invention, it is possible to provide an optical electric field sensor having a characteristic stable for a long time, inasmuch as invasion of a foreign substance is avoided during application of silicone. Since no special facility is required and the operation itself is very easy, no substantial increase in process time is required. (Fourth Example) Fig. 10 shows an optical electric field sensor according to the fourth example. Referring to Fig. 10, a Mach-Zehnder interferometer pattern similar to the conventional one illustrated in Fig. 2 was formed on a Z-cut substrate 21 of LiNbO 3 crystal by a Ti pattern. Then, an optical waveguide 12 was formed by thermal diffusion. Thereafter, an SiO 2 film was formed on a surface of the optical waveguide 12. A pattern of modulation electrodes 22 was formed thereon. For input and output of a laser beam, the optical waveguide was subjected to face polishing. A constant polarization optical fiber 3 and a single mode fiber 4 were connected to a light incident side and a light outgoing side, respectively. The element thus manufactured has an optical modulation characteristic as illustrated in Fig. 3, like in the conventional case. The foregoing structure is similar to that of the conventional case. Thereafter, according to the fourth example, antennas 2 for electric field detection were connected to the modulation electrodes 22. An entire arrangement was packaged as illustrated in Fig. 10. The antennas are not illustrated in Fig. 10. The package was made up by the use of an organic adhesive and sealed so that the internal element is not affected by an outside air. By the use of two kinds of vinyl chloride plates, namely, a vinyl chloride plate subjected to the antistatic treatment according to the fourth example and a comparative vinyl chloride plate not subjected to any treatment, the packages were individually made up and subjected to measurement of electric charge. At first, the above-mentioned two kinds of packages were applied with electric fields of a same intensity. After lapse of a predetermined time duration, electric charges were measured and compared with each other. As a result, after 30 seconds from application of the electric field, no substantial electric charge was observed in the antistatic-treated package according to the sixth embodiment of this invention. On the other hand, in the package of the comparative example without any treatment, the electric charge was measured to correspond to approximately a half of the intensity of the applied electric field. The above-mentioned result shows that the optical electric field sensor using the package according to the fourth example is capable of carrying out optical modulation of an electric field to be measured alone. This is because no disturbance or influence is given to the ambient electric field by electrification of the package. In addition, according to the fourth example, it is possible to provide the optical electric field sensor which is capable of removing an electrostatic field from the package material after packaging so as not to disturb the electric field to be measured. According to the fourth example, it is possible to provide the optical electric field sensor which is capable of measuring the electric field free from an influence of disturbance by removing the electrostatic field generated from the package material even if the plastic material is used. According to the fourth example, it is possible to provide the optical electric field sensor which has an excellent temperature characteristic, by suppressing the influence of the variation of the ambient temperature around the optical electric field sensor upon the optical crystal of the optical modulator. According to the fourth example, it is possible not only to contribute to improvement of the temperature characteristic of the optical electric field sensor, which has been a problem in prior art, but also to provide the optical electric field sensor manufactured at a relatively low cost in a reduced process time with a high productivity. As described above, it is possible to provide the optical electric field sensor having a structure of suppressing heat conduction of thermal fluctuation outside of the optical electric field sensor to the optical crystal so that any device of a high accuracy is unnecessary and the temperature characteristic is improved. (Industrial Application Field) As described above, the electric field sensor according to this invention is adapted to measurement of an electric field intensity within a spatial field, typically, EMC measurement (noise measurement).

Claims: An optical electric field sensor which comprises: at least a pair of modulation electrodes (13) located in the vicinity of an optical waveguides (12) formed on an optical crystal substrate (11) having an electrooptical effect and which is for measuring an electric field intensity by use of variation of at least one of an intensity, a phase, and a polarization direction of a light beam, said variation being caused by leading to said pair of modulation electrodes (13) an electric field spontaneously or forcedly generated; characterized in that conductive resin (14) is applied onto the entire surface of said optical crystal substrate (11) and/or silicone (17) is applied between said modulation electrodes (13). An optical electric field sensor as claimed in claim 1, wherein said optical crystal substrate (11) is fixedly surrounded by a heat insulation material (5).

Inventors: TANABE TAKANOBU, TOKANO YUICHI, TANABE, TAKANOBU, TOKANO, YUICHI, Tanabe, Takanobu, c/o Tokin Corporation, Tokano, Yuichi, c/o Tokin Corporation
Applicants: NEC TOKIN CORP, NEC TOKIN CORPORATION
Application year: 1994
Main classification: G01R29
IPC codes: G01R29